Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Topological textures in Zr-substituted barium titanate

Florian Mayer*

  • *Contact author: florian.mayer@mcl.at

Phys. Rev. B 113, 054111 – Published 17 February, 2026

DOI: https://doi.org/10.1103/cprh-l3mx

Abstract

Topological polarization textures in ferroelectrics offer pathways to dense memory, neuromorphic computing, and controlled probes of topology in solids. In rhombohedral barium titanate, theory has identified stable antiskyrmions of topological charge −2 that fractionalize into six −1/3 hotspots, termed topological quarks. Here, we extend this landscape to Zr-substituted barium titanate (BZT) using a first-principles parameterized effective Hamiltonian framework. In an ordered 12.5% composition, the chemically doubled periodicity enforces an alternation along [111]: one half hosts the −2 antiskyrmion (six −1/3 quarks), the other a +4 skyrmion (six +2/3 quarks). The two share the same six-vortex scaffold (threefold motif) but differ in the core-level polarization texture, resulting in an integer +1 per vortex offset in the plane-integrated (slice) topological charge. In random BZT, nanodomains remain inducible and cryogenically stable, yet quenched disorder pins and distorts the vortices, producing a heterogeneous, skyrmion-glass–like state with fluctuations of the topological charge along the nanodomain axis. Thermal stability maps show that pure barium titanate retains −2 textures up to ∼100 K, whereas in BZT the collapse temperature is nonmonotonic, with a minimum near 6–8% Zr, reflecting competition between ferroelectric softening and disorder pinning. Importantly, the 12.5% ordered arrangement remains rhombohedral above 300 K, enabling field-stabilized nanodomains at 293 K. Under a local [111] bias, the ordered system carries +4 slice charge, while the random composition fragments under the same conditions. These results establish BZT as a platform for chemically programmed, fractionalized ferroelectric topology from cryogenic to room temperature and suggest routes to multistate, reconfigurable devices.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (55)

  1. C. Back, V. Cros, H. Ebert, K. Everschor-Sitte, A. Fert, M. Garst, T. Ma, S. Mankovsky, T. L. Monchesky, M. Mostovoy, et al., The 2020 skyrmionics roadmap, J. Phys. D. Appl. Phys. 53, 363001 (2020).
  2. A. Fert, N. Reyren, and V. Cros, Magnetic skyrmions: Advances in physics and potential applications, Nat. Rev. Mater. 2, 17031 (2017).
  3. S. Mühlbauer, B. Binz, F. Jonietz, C. Pfleiderer, A. Rosch, A. Neubauer, R. Georgii, and P. Böni, Skyrmion lattice in a chiral magnet, Science 323, 915 (2009).
  4. S. Seki and M. Mochizuki, Skyrmions in Magnetic Materials, 1st ed. (Springer International Publishing, Cham, Switzerland, 2015).
  5. T. Schulz, R. Ritz, A. Bauer, M. Halder, M. Wagner, C. Franz, C. Pfleiderer, K. Everschor, M. Garst, and A. Rosch, Emergent electrodynamics of skyrmions in a chiral magnet, Nat. Phys. 8, 301 (2012).
  6. U. K. Rößler, A. N. Bogdanov, and C. Pfleiderer, Spontaneous skyrmion ground states in magnetic metals, Nature (London) 442, 797 (2006).
  7. S. Heinze, K. von Bergmann, M. Menzel, J. Brede, A. Kubetzka, R. Wiesendanger, G. Bihlmayer, and S. Blügel, Spontaneous atomic-scale magnetic skyrmion lattice in two dimensions, Nat. Phys. 7, 713 (2011).
  8. A. K. Nayak, V. Kumar, T. Ma, P. Werner, E. Pippel, R. Sahoo, F. Damay, U. K. Rößler, C. Felser, and S. S. P. Parkin, Magnetic antiskyrmions above room temperature in tetragonal Heusler materials, Nature (London) 548, 561 (2017).
  9. R. Zhu, Z. Jiang, X. Zhang, X. Zhong, C. Tan, M. Liu, Y. Sun, X. Li, R. Qi, K. Qu, Z. Liu, M. Wu, M. Li, B. Huang, Z. Xu, J. Wang, K. Liu, P. Gao, J. Wang, J. Li, and X. Bai, Dynamics of polar skyrmion bubbles under electric fields, Phys. Rev. Lett. 129, 107601 (2022).
  10. S. Das, Z. Hong, V. A. Stoica, M. A. P. Gonçalves, Y. T. Shao, E. Parsonnet, E. J. Marksz, S. Saremi, M. R. McCarter, A. Reynoso, et al., Local negative permittivity and topological phase transition in polar skyrmions, Nat. Mater. 20, 194 (2021).
  11. S. Das, Y. L. Tang, Z. Hong, M. A. P. Gonçalves, M. R. McCarter, C. Klewe, K. X. Nguyen, F. Gómez-Ortiz, P. Shafer, E. Arenholz, et al., Observation of room-temperature polar skyrmions, Nature (London) 568, 368 (2019).
  12. A. K. Yadav, C. T. Nelson, S.-L. Hsu, Z. Hong, J. D. Clarkson, C. M. Schlepütz, A. R. Damodaran, P. Shafer, E. Arenholz, L. R. Dedon, et al., Observation of polar vortices in oxide superlattices, Nature (London) 530, 198 (2016).
  13. Z. Hong, A. R. Damodaran, F. Xue, S.-L. Hsu, J. Britson, A. K. Yadav, C. T. Nelson, J.-J. Wang, J. F. Scott, L. W. Martin, R. Ramesh, and L.-Q. Chen, Stability of polar vortex lattice in ferroelectric superlattices, Nano Lett. 17, 2246 (2017).
  14. V. Stepkova and J. Hlinka, Creation, annihilation and transport of nonmagnetic antiskyrmions within Ginzburg–Landau–Devonshire model, J. Appl. Phys. 137, 034102 (2025).
  15. F. Mayer and J. Hlinka, Thermal stability and topological charge fragmentation in antiskyrmions of rhombohedral barium titanate, Phys. Rev. B 111, 174106 (2025).
  16. F. Gómez-Ortiz, L. Bastogne, S. Anand, M. Yu, X. He, and P. Ghosez, Switchable skyrmion–antiskyrmion tubes in rhombohedral BaTiO3 and related materials, Phys. Rev. B 111, L180104 (2025).
  17. C. Halcrow and E. Babaev, Fractional skyrme lines in ferroelectric barium titanate, Phys. Rev. Res. 6, L032011 (2024).
  18. M. A. P. Gonçalves, C. Escorihuela-Sayalero, P. Garca-Fernández, J. Junquera, and J. Íñiguez, Theoretical guidelines to create and tune electric skyrmion bubbles, Sci. Adv. 5, eaau7023 (2019).
  19. H. Aramberri and J. Íñiguez-González, Brownian electric bubble quasiparticles, Phys. Rev. Lett. 132, 136801 (2024).
  20. M. A. P. Gonçalves, M. Paściak, and J. Hlinka, Antiskyrmions in ferroelectric barium titanate, Phys. Rev. Lett. 133, 066802 (2024).
  21. M. Eremenko, V. Krayzman, S. Gorfman, A. Bosak, H. Y. Playford, P. A. Chater, B. Ravel, W. J. Laws, F. Ye, A. Minelli, et al., Emergent topological polarization textures in relaxor ferroelectrics, Nat. Commun. 16, 7531 (2025).
  22. Y. Li, Y. Wei, R. Guo, Y. Wang, H. Zhang, T. Taniguchi, K. Watanabe, Y. Shi, Y. Shi, C. Wang, and Z. Fei, Unusual topological polar texture in moiré ferroelectrics, Nat. Commun. 16, 5451 (2025).
  23. L. Gao, Y. Shen, S. Prokhorenko, Y. Nahas, and L. Bellaiche, Poincaré sphere engineering of dynamical ferroelectric topological solitons, Phys. Rev. B 112, L121102 (2025).
  24. I. A. Lukyanchuk, A. G. Razumnaya, S. Kondovych, Y. A. Tikhonov, B. Khesin, and V. M. Vinokur, Topological foundations of ferroelectricity, Phys. Rep. 1110, 1 (2025).
  25. J. Junquera, Y. Nahas, S. Prokhorenko, L. Bellaiche, J. Íñiguez, D. G. Schlom, L.-Q. Chen, S. Salahuddin, D. A. Muller, L. W. Martin, and R. Ramesh, Topological phases in polar oxide nanostructures, Rev. Mod. Phys. 95, 025001 (2023).
  26. M. Hassan, S. Koraltan, A. Ullrich, F. Bruckner, R. O. Serha, K. V. Levchenko, G. Varvaro, N. S. Kiselev, M. Heigl, C. Abert, D. Suess, and M. Albrecht, Dipolar skyrmions and antiskyrmions of arbitrary topological charge at room temperature, Nat. Phys. 20, 615 (2024).
  27. F. Mayer, M. N. Popov, P. Ondrejkovic, J. Hlinka, J. Spitaler, and M. Deluca, Finite-temperature investigation of homovalent and heterovalent substituted BaTiO3 from first principles, Phys. Rev. B 106, 224109 (2022).
  28. C. Mentzer, S. Lisenkov, Z. G. Fthenakis, and I. Ponomareva, Phase evolution in the ferroelectric relaxor Ba(T1−xZrx)O3 from atomistic simulations, Phys. Rev. B 99, 064111 (2019).
  29. J. Petzelt, V. Bovtun, D. Nuzhnyy, M. Kempa, M. Savinov, M. Paściak, S. Kamba, G. Canu, and V. Buscaglia, Broadband dielectric, terahertz, and infrared spectroscopy of BaTiO3−BaZrO3 solid solution: From proper ferroelectric over diffuse and relaxor ferroelectrics and dipolar glass to normal dielectric, Phys. Status Solidi (B) 258, 2100259 (2021).
  30. W. Zhong, D. Vanderbilt, and K. M. Rabe, First-principles theory of ferroelectric phase transitions for perovskites: The case of BaTiO3, Phys. Rev. B 52, 6301 (1995).
  31. U. V. Waghmare and K. M. Rabe, Ab initio statistical mechanics of the ferroelectric phase transition in PbTiO3, Phys. Rev. B 55, 6161 (1997).
  32. L. Bellaiche, A. García, and D. Vanderbilt, Finite-temperature properties of Pb(Zr1−xTix)O3 alloys from first principles, Phys. Rev. Lett. 84, 5427 (2000).
  33. L. Bellaiche, A. García, and D. Vanderbilt, Low-temperature properties of Pb(Zr1−xTix)O3 solid solutions near the morphotropic phase boundary, Ferroelectrics 266, 41 (2002).
  34. T. Nishimatsu, U. V. Waghmare, Y. Kawazoe, and D. Vanderbilt, Fast molecular-dynamics simulation for ferroelectric thin-film capacitors using a first-principles effective Hamiltonian, Phys. Rev. B 78, 104104 (2008).
  35. T. Nishimatsu, M. Iwamoto, Y. Kawazoe, and U. V. Waghmare, First-principles accurate total energy surfaces for polar structural distortions of BaTiO3, PbTiO3, and SrTiO3: Consequences for structural transition temperatures, Phys. Rev. B 82, 134106 (2010).
  36. A. Paul, J. Sun, J. P. Perdew, and U. V. Waghmare, Accuracy of first-principles interatomic interactions and predictions of ferroelectric phase transitions in perovskite oxides: Energy functional and effective hamiltonian, Phys. Rev. B 95, 054111 (2017).
  37. F. Mayer, M. Deluca, and M. N. Popov, Hidden phases in homovalent and heterovalent substituted BaTiO3, Phys. Rev. B 107, 184307 (2023).
  38. F. Mayer, M. N. Popov, D. M. Evans, S. Krohns, M. Deluca, and J. Spitaler, Improved description of the potential energy surface in BaTiO3 by anharmonic phonon coupling, Phys. Rev. B 106, 064108 (2022).
  39. See Supplemental Material at http://link.aps.org/supplemental/10.1103/cprh-l3mx for additional details on the effective-Hamiltonian model, the 12.5% superlattice geometry, Bloch-point–like conversion signatures, the topological charge-difference analysis, and complementary supporting results.
  40. S. D. Bond, B. J. Leimkuhler, and B. B. Laird, The Nosé-Poincaré method for constant temperature molecular dynamics, J. Comput. Phys. 151, 114 (1999).
  41. B. Berg and M. Lüscher, Definition and statistical distributions of a topological number in the lattice O(3) σ-model, Nucl. Phys. B. 190, 412 (1981).
  42. C. Heo, N. S. Kiselev, A. K. Nandy, S. Blügel, and T. Rasing, Switching of chiral magnetic skyrmions by picosecond magnetic field pulses via transient topological states, Sci. Rep. 6, 27146 (2016).
  43. P. E. Blöchl, Projector augmented-wave method, Phys. Rev. B 50, 17953 (1994).
  44. G. Kresse and J. Hafner, Ab initio molecular-dynamics simulation of the liquid-metal–amorphous-semiconductor transition in germanium, Phys. Rev. B 49, 14251 (1994).
  45. G. Kresse and J. Furthmüller, Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set, Phys. Rev. B 54, 11169 (1996).
  46. G. Kresse and J. Furthmüller, Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set, Comput. Mater. Sci. 6, 15 (1996).
  47. G. Kresse and D. Joubert, From ultrasoft pseudopotentials to the projector augmented-wave method, Phys. Rev. B 59, 1758 (1999).
  48. G. I. Csonka, J. P. Perdew, A. Ruzsinszky, P. H. T. Philipsen, S. Lebègue, J. Paier, O. A. Vydrov, and J. G. Ángyán, Assessing the performance of recent density functionals for bulk solids, Phys. Rev. B 79, 155107 (2009).
  49. Y.-J. Wang, Y.-P. Feng, Y.-L. Tang, Y.-L. Zhu, Y. Cao, M.-J. Zou, W.-R. Geng, and X.-L. Ma, Polar bloch points in strained ferroelectric films, Nat. Commun. 15, 3949 (2024).
  50. D. Wolf, S. Schneider, U. K. Rößler, A. Kovács, M. Schmidt, R. E. Dunin-Borkowski, B. Büchner, B. Rellinghaus, and A. Lubk, Unveiling the three-dimensional magnetic texture of skyrmion tubes, Nat. Nanotechnol. 17, 250 (2022).
  51. Y. Li, L. Pierobon, M. Charilaou, H.-B. Braun, N. R. Walet, J. F. Löffler, J. J. Miles, and C. Moutafis, Tunable terahertz oscillation arising from Bloch-point dynamics in chiral magnets, Phys. Rev. Res. 2, 033006 (2020).
  52. S. Hoshino and N. Nagaosa, Theory of the magnetic skyrmion glass, Phys. Rev. B 97, 024413 (2018).
  53. E. M. Chudnovsky and D. A. Garanin, Skyrmion glass in a 2D Heisenberg ferromagnet with quenched disorder, New J. Phys. 20, 033006 (2018).
  54. O. Diéguez, S. Tinte, A. Antons, C. Bungaro, J. B. Neaton, K. M. Rabe, and D. Vanderbilt, Ab initio study of the phase diagram of epitaxial BaTiO3, Phys. Rev. B 69, 212101 (2004).
  55. J. Junquera and P. Ghosez, Critical thickness for ferroelectricity in perovskite ultrathin films, Nature (London) 422, 506 (2003).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation